JPH0550713U - Transformer - Google Patents

Transformer

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Publication number
JPH0550713U
JPH0550713U JP10084091U JP10084091U JPH0550713U JP H0550713 U JPH0550713 U JP H0550713U JP 10084091 U JP10084091 U JP 10084091U JP 10084091 U JP10084091 U JP 10084091U JP H0550713 U JPH0550713 U JP H0550713U
Authority
JP
Japan
Prior art keywords
transformer
iron core
output
current
magnetic flux
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP10084091U
Other languages
Japanese (ja)
Inventor
実 大辺
研 鍋谷
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Meidensha Corp
Original Assignee
Meidensha Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Meidensha Corp filed Critical Meidensha Corp
Priority to JP10084091U priority Critical patent/JPH0550713U/en
Publication of JPH0550713U publication Critical patent/JPH0550713U/en
Pending legal-status Critical Current

Links

Abstract

(57)【要約】 (修正有) 【目的】 鉄心部に磁路と交わる方向に伸びるスリット
穴を設けることにより、小形で騒音や損失の小さい変圧
器を得る。 【構成】 鉄心脚2u,2v,2wあるいはヨーク1
a,1bに、磁束の流れる方向に対して所定の角度を持
って伸びるように1個なしいは複数個のスリット穴6を
設けたものである。
(57) [Summary] (Modified) [Purpose] A small transformer with low noise and loss is obtained by providing a slit hole in the core that extends in the direction intersecting the magnetic path. [Structure] Iron core legs 2u, 2v, 2w or yoke 1
Each of a and 1b is provided with one or a plurality of slit holes 6 so as to extend at a predetermined angle with respect to the magnetic flux flowing direction.

Description

【考案の詳細な説明】[Detailed description of the device]

【0001】[0001]

【産業上の利用分野】[Industrial applications]

本考案は変圧器に係り、特に電力変換装置に用いて有効な変圧器に関する。 The present invention relates to a transformer, and more particularly to a transformer effective for use in a power conversion device.

【0002】[0002]

【従来の技術】[Prior Art]

直流から交流を得る手法として、PWM方式が一般的に用いられている。この PWM方式では、交流出力電圧に多少の直流分が含まれている。この直流分は、 半導体素子の順方向電圧降下(VF特性)のバラツキや、上下アームの短絡を防 止するためのデッドタイムのバラツキ、あるいは直流ラインの電圧変動時に起因 している。PWM方式を採用したインバータに於いて、その交流出力ラインに変 圧器(通称インバータ変圧器という)があると、この直流分のために、変圧器鉄 心が飽和し、インバータの交流出力電流が急激に増加したり、あるいは、変圧器 二次側の出力電圧が減少するため、出力電圧が変動したりすることがある。 The PWM method is generally used as a method for obtaining alternating current from direct current. In this PWM method, the AC output voltage contains some DC component. This direct current component is caused by variations in the forward voltage drop (VF characteristic) of the semiconductor element, variations in dead time for preventing a short circuit between the upper and lower arms, or variations in the voltage of the direct current line. In an inverter that employs the PWM method, if there is a transformer (commonly called an inverter transformer) in the AC output line, the transformer core is saturated due to this DC component, and the AC output current of the inverter suddenly increases. May increase or the output voltage on the secondary side of the transformer may decrease, causing the output voltage to fluctuate.

【0003】 現在、この直流分によるインバータ変圧器の偏磁を防止するため、交流出力ラ インに直流分が計測可能な電流検出器をとりつけ、交流ラインの直流電流分を検 出し、この量が減少する様にフィードバック制御をかけている。At present, in order to prevent the magnetic bias of the inverter transformer due to this DC component, a current detector capable of measuring the DC component is attached to the AC output line, and the DC current component of the AC line is detected. Feedback control is applied so as to decrease.

【0004】 すなわち、図10は従来の定電圧定周波数電源装置(CVCF装置)の直流偏 磁防止装置を示す。同図において1は直流電源、2a〜2dは半導体スイッチ素 子、3は出力変圧器、4はコイル、5はコンデンサでこれらのコイル4とコンデ ンサ5によって交流フィルタ回路6が形成され、直流電源1,半導体スイッチ素 子2a〜2d,出力変圧器3および交流フィルタ回路6によって主回路が構成さ れる。 このような主回路構成のCVCFにおいて、電圧変成器7により出力電 圧を検出し、その検出電圧を整流器8で整流し、この電圧値を突合せ回路9で設 定電圧値Vsetと比較し、増幅回路10により誤差増幅し、それと基準正弦波 発生器11の出力を掛算器12にて掛け合せる。掛算器12の出力と三角波発生 器13の出力をコンパレータ14にて大小比較し、制御信号Sa〜Sdを作って いる。また、出力変圧器3の一次電流を電流変成器15で検出し、その検出電流 をローパスフィルタ16を通すことにより、直流成分を検出し、この値を設定電 流値Isetと比較し、増幅回路17により誤差増幅し、突合せ回路18で掛算 器12の出力をバイアスする事により、出力変圧器3の直流成分を制御している 。なお、図2には単相出力のCVCFについて示したが、三相出力のCVCFに も同様に適用可能である。That is, FIG. 10 shows a DC bias prevention apparatus of a conventional constant voltage constant frequency power supply (CVCF apparatus). In the figure, 1 is a DC power source, 2a to 2d are semiconductor switch elements, 3 is an output transformer, 4 is a coil, 5 is a capacitor, and an AC filter circuit 6 is formed by these coils 4 and a capacitor 5, and a DC power source. 1, the semiconductor switch elements 2a to 2d, the output transformer 3 and the AC filter circuit 6 constitute a main circuit. In the CVCF having such a main circuit configuration, the output voltage is detected by the voltage transformer 7, the detected voltage is rectified by the rectifier 8, and this voltage value is compared with the set voltage value Vset by the matching circuit 9 and amplified. The error is amplified by the circuit 10, and the output of the reference sine wave generator 11 is multiplied by the multiplier 12. The output of the multiplier 12 and the output of the triangular wave generator 13 are compared in magnitude by a comparator 14 to generate control signals Sa to Sd. Further, the primary current of the output transformer 3 is detected by the current transformer 15, and the detected current is passed through the low-pass filter 16 to detect the direct current component, and this value is compared with the set current value Iset, and the amplification circuit The error component 17 is used for error amplification, and the matching circuit 18 biases the output of the multiplier 12 to control the DC component of the output transformer 3. Although FIG. 2 shows a CVCF having a single-phase output, it can be similarly applied to a CVCF having a three-phase output.

【0005】 上記電力変換装置に用いられる変圧器では、装置の小形化、低損失化のため、 鉄心は方向性けい素鋼板を用い、磁束密度も商用変圧器と同等程度近く迄上げて いる。方向性けい素鋼板を用いた変圧器の励磁電流は少なく、かつ、鉄板飽和磁 束密度の2.1Tに対し、1.9T程度から急増する傾向がある。上述した変圧 器を用いる方向にあるが、この様な鉄板特性のため、わずかな直流電流により容 易に鉄心が飽和してしまう。鉄心磁束密度が1.9Tを超えると、急激に励磁電 流が増加する非線形特性由に、出力電圧が安定しないという問題や、励磁電流の 急増による過電流現象が発生する(励磁特性を図5に示す)。In the transformer used in the above power converter, in order to downsize the device and reduce the loss, the core is made of grain-oriented silicon steel sheet and the magnetic flux density is increased to about the same level as that of the commercial transformer. The exciting current of the transformer using the grain-oriented silicon steel plate is small, and the iron plate saturation magnetic flux density of 2.1T tends to rapidly increase from about 1.9T. Although there is a tendency to use the above-mentioned transformer, due to such iron plate characteristics, the iron core is easily saturated by a slight DC current. When the iron core magnetic flux density exceeds 1.9T, the problem that the output voltage is not stable due to the non-linear characteristic that the exciting current increases rapidly and the overcurrent phenomenon due to the rapid increase of the exciting current occur (Fig. Shown in).

【0006】 従来はこのような現象を避けるために、図6と図7に示すような構造としてい た。すなわち、図6と図7において1a,1bはヨーク、2u,2v,2wはヨ ーク1aと1b間に形成された脚部で、3a〜3cは各脚部2u〜2wのほぼ中 央部に設けられたギャップ、4a〜4cはヨーク1aと脚部2u〜2w間に設け られたギャップ、5a〜5cは脚部2u〜2wとヨーク1b間に設けられたギャ ップで、これらのギャップは適宜に組合せて設けられていた。これにより、励磁 電流を定格電流の10〜20%と大きくし、かつ鉄心の磁束密度も1.0ターン (1T)程度とし、予期される直流電圧成分に対し、直流偏磁しない変圧器構造 としていた。Conventionally, in order to avoid such a phenomenon, the structure shown in FIGS. 6 and 7 is used. That is, in FIGS. 6 and 7, 1a and 1b are yokes, 2u, 2v and 2w are leg portions formed between the yokes 1a and 1b, and 3a to 3c are substantially central portions of the leg portions 2u to 2w. Gaps 4a to 4c are provided between the yoke 1a and the legs 2u to 2w, and 5a to 5c are gaps provided between the legs 2u to 2w and the yoke 1b. Were provided in an appropriate combination. As a result, the exciting current is increased to 10 to 20% of the rated current, the magnetic flux density of the iron core is set to about 1.0 turn (1T), and a transformer structure that does not cause DC bias to the expected DC voltage component is provided. I was there.

【0007】[0007]

【考案が解決しようとする課題】[Problems to be solved by the device]

図6,7に示すような変圧器では、図8と図9に示すよう鉄心励磁特性となり 、幾分その特性が改良される。しかしながら、このような変圧器では、寸法,損 失が大きく、またヨークと脚部間のギャップにより騒音が大きくなる等の欠点が あった。 In the transformer as shown in FIGS. 6 and 7, the core excitation characteristics are obtained as shown in FIGS. 8 and 9, and the characteristics are improved to some extent. However, such a transformer has drawbacks such as large size and loss, and increased noise due to the gap between the yoke and the leg.

【0008】 本考案は上述の問題点に鑑みてなされたもので、その目的は鉄心部に磁路と交 わる方向に伸びるスリット穴を設けることにより、小形で騒音や損失の小さい変 圧器を提供することである。The present invention has been made in view of the above problems, and an object thereof is to provide a small-sized transformer with small noise and loss by providing a slit hole extending in a direction intersecting with a magnetic path in an iron core portion. It is to be.

【0009】[0009]

【課題を解決するための手段】[Means for Solving the Problems]

本考案は、上記目的を達成するために、ヨークと脚部からなる鉄心を備えた変 圧器において、前記鉄心に該鉄心に形成される磁路に対して所定角度を持つスリ ット穴を設けて構成したことを特徴とする。 In order to achieve the above object, the present invention provides a transformer having an iron core composed of a yoke and legs, wherein the iron core is provided with a slit hole having a predetermined angle with respect to a magnetic path formed in the iron core. It is characterized in that it is configured.

【0010】[0010]

【作用】[Action]

鉄心磁束密度が増加するにつれて、等価的にギャップに相当するものが大きく なることになり、急激な励磁電流の増加が防止される。 As the iron core magnetic flux density increases, the equivalent equivalent of the gap becomes larger, and a sudden increase in the exciting current is prevented.

【0011】[0011]

【実施例】【Example】

以下に本考案の実施例を図1〜図5を参照しながら説明する。 An embodiment of the present invention will be described below with reference to FIGS.

【0012】 図1は本考案の第1実施例による変圧器の正面図、図2は側面図であって、図 6,図7のものと同一又は相当部分には同一符号が付されている。本実施例にお いては、図1と図2に示すように脚部2u〜2wに、それぞれ、変圧器の励磁時 に形成される磁路に対してほぼ直交する方向に伸びるスリット状の穴6が設けら れている。FIG. 1 is a front view of a transformer according to a first embodiment of the present invention, FIG. 2 is a side view thereof, and the same or corresponding parts as those of FIGS. 6 and 7 are designated by the same reference numerals. .. In this embodiment, as shown in FIGS. 1 and 2, the leg portions 2u to 2w each have a slit-shaped hole extending in a direction substantially orthogonal to the magnetic path formed when the transformer is excited. 6 are provided.

【0013】 上記構成の変圧器においては穴6を設けたことにより、鉄心磁束密度が増加す るにつれ、等価的に鉄心のギャップが大きくなることになる。By providing the holes 6 in the transformer having the above structure, the iron core gap is equivalently increased as the iron core magnetic flux density is increased.

【0014】 具体的には断面P−Qの平均磁束密度は1.6T程度としておき、この時の断 面P′−Q′の平均磁束密度を1.9T程度としておく。直流分がなければ鉄心 の励磁電流は小さい。直流分が発生し、0.2T程度鉄心が偏磁したとすると、 断面P−Qの平均磁束密度は最大1.8T程度であるが断面P′−Q′の平均磁 束密度は2.1Tとなり飽和する。これは鉄心に等価的にギャップが出来たのと 同じで励磁電流は増加する。さらに偏磁するとスリット部分の飽和領域が増加し 、ギャップ長が増加したのと等価となる。Specifically, the average magnetic flux density of the cross section P-Q is set to about 1.6T, and the average magnetic flux density of the cross section P'-Q 'at this time is set to about 1.9T. If there is no direct current component, the exciting current of the iron core is small. If a direct current is generated and the iron core is demagnetized by about 0.2T, the average magnetic flux density of the cross section P-Q is about 1.8T at maximum, but the average magnetic flux density of the cross section P'-Q 'is 2.1T. Becomes saturated. This is the same as when a gap was created equivalently in the iron core, and the exciting current increases. Further demagnetization increases the saturation region of the slit, which is equivalent to increasing the gap length.

【0015】 スリットがない変圧器では、直流偏磁すると鉄心全体が飽和してしまうため、 急激な励磁電流の増加が生じるが、スリットがある変圧器ではスリット部のみが 飽和し、スリットのないものは未飽和なため、急激な励磁電流の増加は発生しな い。図5にスリットありのインバータ変圧器の励磁特性を示す。これにより、安 定な制御が実現可能である。In a transformer without slits, when the DC bias is magnetized, the entire iron core saturates, which causes a rapid increase in the exciting current. However, in transformers with slits, only the slits are saturated and those without slits Since is not saturated, there is no sudden increase in exciting current. Fig. 5 shows the excitation characteristics of the inverter transformer with slits. As a result, stable control can be realized.

【0016】 以上のように本実施例によれば、インバータ変圧器鉄心脚にスリットを入れる ことにより、(1)インバータ変圧器の鉄心磁束密度を上げることができるため 、インバータ変圧器の小形化、低損失化が達成できる。(2)従来のヨーク、脚 間にギャップを設ける必要がなく、そのため騒音を低減することが可能である。 (3)直流偏磁の制御が安定に行え、従来発生していたインバータ交流ラインの 過電流や、出力電圧の変動をなくすことが可能である。As described above, according to this embodiment, by slitting the core legs of the inverter transformer, (1) the magnetic flux density of the iron core of the inverter transformer can be increased. Low loss can be achieved. (2) Since it is not necessary to provide a gap between the conventional yoke and legs, it is possible to reduce noise. (3) DC bias magnetism can be stably controlled, and it is possible to eliminate the overcurrent of the inverter AC line and the fluctuation of the output voltage that have been conventionally generated.

【0017】 図3と図4は本考案の第2実施例による変圧器を示すもので、本実施例におい てはヨーク1aと1bの磁路が形成される部位に、該磁路に対してほぼ直交する 方向に伸びるスリット穴7が形成されており、図1,図2のものと同様な作用, 効果が得られる。3 and 4 show a transformer according to a second embodiment of the present invention. In this embodiment, the magnetic paths of the yokes 1a and 1b are formed at the portions where the magnetic paths are formed. A slit hole 7 extending in a substantially orthogonal direction is formed, and the same action and effect as those of FIGS. 1 and 2 can be obtained.

【0018】[0018]

【考案の効果】[Effect of the device]

本考案は、以上の如くであって、鉄心脚あるいはヨークに、磁束の流れる方向 に対して所定の角度を持って伸びるように1個なしいは複数個のスリット穴を設 けたものであるから、インバータの出力変圧器として用いると、その励磁特性を 、インバータが発生する直流分に対して、鉄心の飽和による励磁電流の急激な増 加を抑制するようにでき、小形にして騒音と損失を低減した変圧器が得られる。 The present invention is as described above, and one or more slit holes are provided in the iron core leg or the yoke so as to extend at a predetermined angle with respect to the magnetic flux flowing direction. When used as an output transformer of an inverter, its excitation characteristics can suppress the rapid increase of the excitation current due to the saturation of the iron core with respect to the direct current component generated by the inverter, making it compact and reducing noise and loss. A reduced transformer is obtained.

【図面の簡単な説明】[Brief description of drawings]

【図1】本考案の第1実施例による変圧器の正面図。FIG. 1 is a front view of a transformer according to a first embodiment of the present invention.

【図2】図1の変圧器の側面図。2 is a side view of the transformer of FIG. 1. FIG.

【図3】本考案の第2実施例による変圧器の正面図。FIG. 3 is a front view of a transformer according to a second embodiment of the present invention.

【図4】図3の変圧器の側面図。4 is a side view of the transformer of FIG.

【図5】本考案の実施例による変圧器の鉄心励磁特性
図。
FIG. 5 is an iron core excitation characteristic diagram of a transformer according to an embodiment of the present invention.

【図6】従来の変圧器の正面図。FIG. 6 is a front view of a conventional transformer.

【図7】図6の変圧器の側面図。7 is a side view of the transformer of FIG.

【図8】従来の変圧器の鉄心励磁特性図。FIG. 8 is an iron core excitation characteristic diagram of a conventional transformer.

【図9】従来の変圧器の鉄心励磁特性図。FIG. 9 is an iron core excitation characteristic diagram of a conventional transformer.

【図10】電力変換装置の制御装置のブロック図。FIG. 10 is a block diagram of a control device of the power conversion device.

【符号の説明】[Explanation of symbols]

1a,1b…ヨーク、2u,2v,2w…鉄心脚、6,
7…スリット穴。
1a, 1b ... Yoke, 2u, 2v, 2w ... Iron core leg, 6,
7 ... Slit hole.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】 ヨークと脚部からなる鉄心を備えた変圧
器において、前記鉄心に該鉄心に形成される磁路に対し
て所定角度を持つスリット穴を設けて構成したことを特
徴とする変圧器。
1. A transformer provided with an iron core composed of a yoke and legs, wherein the iron core is provided with slit holes having a predetermined angle with respect to a magnetic path formed in the iron core. vessel.
JP10084091U 1991-12-09 1991-12-09 Transformer Pending JPH0550713U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10084091U JPH0550713U (en) 1991-12-09 1991-12-09 Transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10084091U JPH0550713U (en) 1991-12-09 1991-12-09 Transformer

Publications (1)

Publication Number Publication Date
JPH0550713U true JPH0550713U (en) 1993-07-02

Family

ID=14284518

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10084091U Pending JPH0550713U (en) 1991-12-09 1991-12-09 Transformer

Country Status (1)

Country Link
JP (1) JPH0550713U (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006351920A (en) * 2005-06-17 2006-12-28 Toyota Motor Corp Reactor
JP2013105774A (en) * 2011-11-10 2013-05-30 Dengensha Mfg Co Ltd Weld transformer and method for manufacturing the same
JP2014183320A (en) * 2013-03-20 2014-09-29 Schneider Toshiba Inverter Europe Sas Choke and power converter

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006351920A (en) * 2005-06-17 2006-12-28 Toyota Motor Corp Reactor
JP2013105774A (en) * 2011-11-10 2013-05-30 Dengensha Mfg Co Ltd Weld transformer and method for manufacturing the same
JP2014183320A (en) * 2013-03-20 2014-09-29 Schneider Toshiba Inverter Europe Sas Choke and power converter

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